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8.8.15 Heat Pump Fluidized Bed Dryer .............................................................................................. 192
8.9 Design Procedu
8.9.1 Design E
8.9.1.18.9.1.2 Sizing of Bed ................................................................................................................ 193
8.9.1.3 Gas Flow Rate ............................................................................................................. 193
8.9.1.4 Mass Balance, Continuous Drying, Well-Mixed Bed................................................... 193 2006 by Taylor & Francis Groupre ................................................................................................................................... 192
quations........................................................................................................................ 192
Residence Time ............................................................................................................ 1928 Fluidized Bed DryersChung Lim Law and Arun S. Mujumdar
CONTENTS
8.1 Introduction ........................................................................................................................................... 174
8.2 Advantages and Limitations of Fluidized Bed Dryers........................................................................... 177
8.3 Heat Transfer in Fluidized Beds ............................................................................................................ 177
8.4 Mathematical Models of Fluidized Bed Drying .................................................................................... 178
8.4.1 Diffusion Model ......................................................................................................................... 178
8.4.2 Empirical Model ......................................................................................................................... 179
8.4.3 Kinetic Model............................................................................................................................. 180
8.4.4 Single-Phase Model .................................................................................................................... 181
8.4.5 Two-Phase Model....................................................................................................................... 181
8.5 Effect of Operating Parameters on Fluidized Bed Drying ..................................................................... 182
8.5.1 Effect of Bed Height ................................................................................................................... 182
8.5.2 Effect of Particle Size.................................................................................................................. 182
8.5.3 Effect of Gas Velocity................................................................................................................. 182
8.5.4 Effect of Bed Temperature ......................................................................................................... 182
8.6 Types of Fluidized Bed Dryers: Classification and Selection................................................................. 182
8.7 Conventional Fluidized Bed Dryers....................................................................................................... 184
8.7.1 Batch Fluidized Bed Dryers........................................................................................................ 184
8.7.2 Semicontinuous Fluidized Bed Dryers........................................................................................ 184
8.7.3 Well-Mixed, Continuous Fluidized Bed Dryers ......................................................................... 184
8.7.4 Plug Flow Fluidized Bed Dryers ................................................................................................ 185
8.8 Modified Fluidized Bed Dryers.............................................................................................................. 185
8.8.1 Multistage and Multiprocess Fluidized Bed Dryers ................................................................... 185
8.8.2 Hybrid Fluidized Bed Dryers ..................................................................................................... 185
8.8.3 Pulsating Fluidized Bed Dryers .................................................................................................. 186
8.8.4 Fluidized Bed Dryers with Immersed Heat Exchangers ............................................................. 187
8.8.5 Mechanically Assisted Fluidized Bed Dryers.............................................................................. 187
8.8.6 Vibrated Fluidized Bed Dryers ................................................................................................... 187
8.8.7 Agitated Fluidized Bed Dryers/Swirl Fluidizers ......................................................................... 188
8.8.8 Fluidized Bed Dryers of Inert Particles ...................................................................................... 188
8.8.9 Spouted Bed Dryers.................................................................................................................... 189
8.8.10 Recirculating Fluidized Bed Dryers.......................................................................................... 190
8.8.11 Jetting Fluidized Bed Dryers .................................................................................................... 190
8.8.12 Fluidized Bed Dryers with Internal Baffles............................................................................... 190
8.8.13 Superheated Steam Fluidized Bed Dryers................................................................................. 191
8.8.14 Fluidized Bed Freeze Dryer ...................................................................................................... 191, LLC.
8.9.1.5 Heat Balance, Continuous Drying, Well-Mixed........................................................... 193
8.9.2 A Sample Design Calculation..................................................................................................... 195
8.10 Conclusion ........................................................................................................................................... 198
Notation ......................................................................................................................................................... 198
References ...................................................................................................................................................... 199
8.1 INTRODUCTION
Fluidized bed dryers (FBD) are used extensively for
the drying of wet particulate and granular materials
that can be fluidized, and even slurries, pastes, and
suspensions that can be fluidized in beds of inert
solids. They are commonly used in processing many
products such as chemicals, carbohydrates, foodstuff,
biomaterials, beverage products, ceramics, pharma-
ceuticals in powder or agglomerated form, health-
care products, pesticides and agrochemicals, dyestuffs
and pigments, detergents and surface-active agents,
fertilizers, polymer and resins, tannins, products for
calcination, combustion, incineration, waste manage-
The bed of particles rests on a gas distributor plate.
The fluidizing gas passes through the distributor and
it is uniformly distributed across the bed. Pressure
drop across the bed increases as the fluidizing gas
velocity is increased. At a certain gas velocity, the
bed is fluidized when the gas stream totally supports
the weight of the whole bed. This state is known as
minimum fluidization and the corresponding gas vel-
ocity is calledminimumfluidization velocity, umf. Pres-
sure drop across the bed remains nearly the same as
pressure drop at minimum fluidization even if the gas
velocity is increased furth er. Figure 8.1 sho ws v arious
regimes of the parti culate bed from packed to bubbling
pe
n
Power consumption High Low Low Medium Medium
Maintenance High Medium Medium Medium Medium
Energy efficiency Medium Medium High High HighEase of control Low Medium High High High
Capacity High Medium Medium Medium High
aFlash dryer is used only for removing surface moisture from smaller particles at relatively short drying times typically in the range of 1030 s.ment processes, and environmental protection pro-
cesses. Fluidized bed operation gives important
advantages such as good solids mixing, high rates of
heat and mass transfer, and easy material transport.
For drying of powders in the particle size range
of 50 to 2000 mm, fluidized beds compete suc-cessfully with other more traditional dryer types,
e.g., rotary, tunnel, conveyor, continuous tray (see
Table 8.1).
Conventional fluidized bed is formed by passing a
gas stream from the bottom of a bed of particulate
solids. At low gas velocities the bed is static (packed).
TABLE 8.1Comparison of Fluidized Bed Dryers (Conventional Tyfor Particulate Solids
Criterion Rotary Flasha
Particle size Large range Fine particles
Particle size distribution Flexible Limited size distributio
Drying time (approx.) Up to 60min 1030 s
Floor area Large Large length
Turndown ratio Large Small
Attrition High High 2006 by Taylor & Francis Group, LLC.bed when the gas velocity is increased. The graphs
show the bed pressure drops and bed voidage under
various regimes.
A fluidized bed is operated at superficial gas vel-
ocities higher than the minimum fluidization velocity,
umf, normally at 24 umf. The minimum fluidiza-
tion velocity is typically obtained from experiments.
There are several ways to determine the minimum
fluidization velocity experimentally. It can also be
estimated using various correlations. A list of min-
imum fluidization velocity can be obtained from
Gupta and Sathiyamoorthy [1]. It should be noted
that these correlations have limitations such as
s and Modified Types) with Other Competing Dryers
Conveyor Conventional FBDs Modified FBDs
500mm10mm 1002000 mm 10mm10mm
Flexible Limited size distribution Wide distribution
Up to 120min Up to 60min Up to 60min
Large Small Small
Small Small Small
Low High High
Expandedbed
Minimumfluidization
Bubblingfluidization
Fixed bed
Pressuredrop
umf Gas velocity
Bedvoidageparticle size, column dimens ions, operati ng param-
eters, etc. Thus , they are va lid in a certa in ran ge of
criteri a and ope rating conditio ns. The effe ct of wet ness
of the parti cles is, howeve r, not included.
Par ticles wi th high initial moisture content require
a higher minimum fluid ization veloci ty than simila r
bed of dry particles . Due to dominant co hesive forces
exerted by wet ted surfa ces, onl y the top layer of the
bed of soli ds is fluidized bed. The bottom layer s may
remain stationar y during the initial stage of dry ing
when the soli ds are quite wet.
For the case of dr y (or parti ally dry, no surface
moisture) particles , if the fluidizin g gas is furth er
increa sed, the be d of particles goes through diff erent
types of fluidiza tion regimes depe nding on the types
of pa rticles wi th refer ence to the Gelda rt class ification
of powder s [2,3]. Based on fluidiza tion quality, pow-
ders can be classified into four group s: group A (aera -
table pa rticles, easy- to-fluid ize when dry), g roup B
(sandlike particles , easy-to-flui dize when dry), group
C (fine and ultr afine particles , difficult- to-fluidize due
to dominat ed cohesiv e forces between particles ), and
group D (larg e and dense pa rticles, poor fluidiza tion
umf Gas velocity
FIGURE 8.1 Various regimes of a bed of particles at differ-ent gas velocities.
2006 by Taylor & Francis Group, LLC.quality due to form ation of large bubbl es in the bed).
Figure 8.2 shows the various fluidiza tion regimes
exhibi ted by a bed of dry parti cles of diff erent class es
with increasing gas velocity. Flu idized bed dryers
are nor mally operate d in the regimes of smoot h and
bubbling fluidiza tion.
After passin g through the fluidized bed, the ga s
stream is intr oduced into gas-cleani ng syste ms to sep-
arate fine particles (dusts) from the exit gas stream
before dischar ging it to the a tmosph ere. Figu re 8.3
shows a typical setup of fluidized bed drying system.
A typical fluidized bed drying system consists of a gas
blower, heater, fluidized bed column, gas-cleaning
systems such as cyclone, bag filters, precipitator, and
scrubber. To save energy, sometimes the exit gas is
partially recycled.
The bubbling fluidized bed (Figure 8.3) is divided
vertically into two zones, namely a dense phase and
a freeboard region (also known as lean phase or
dispersed phase). The dense phase is located at the
bottom; above the dense phase is the freeboard in
which the solids hold-up and density decreases with
height (Figure 8.3).
Fluidizing gas after passing through the bed of
particles enters the freeboard region, and carries
with it fine particles which are terminal velocities
smaller than the operating gas velocity. This phenom-
enon is known as elutriation. Solids hold-up in the
freeboard region decreases as the freeboard height is
increased until a height beyond which the solids hold-
up remains unchanged. This point is known as the
transport disengagement height (TDH). TDH can be
estimated from several empirical correlations; these
correlations are expressed in terms of one or two
operating parameters thus, the predictions are gener-
ally poor. However, there is no universally accep-
ted equation for calculating TDH. As a result, it is
best to determine the transport disengaging height
experimentally.
In designing a fluidized bed dryer for solids dry-
ing, it is important to take note about the occurrence
of entrainment of fine particles, especially if the solids
are polydispersed (i.e., have wide particle size distri-
bution). The gas exit should be placed at a height
above the TDH to minimize elutriation of fines.
On the other hand, by means of fines elutriation,
solids in fluidized bed can be classified into fine and
coarse products. Particles that are elutriated by the
fluidized gas stream are known as fine products
whereas particles retained in the bed are known as
coarse products. This process is called fluidized bed
separation or classification or dedusting. For pro-
cesses that require a certain degree of dedusting (re-
moval of undesirable fine particles) or classification,
operating gas velocity and location of gas exit should
Fixedbed
Turbulent Fast Pneumaticconveying
Smooth Bubbling
# Bubble maximum size greater than 0.66column diameter
Channeling Gas velocity
#
entbe chosen carefully in order to achieve the appropri-
ate product cut size. Cut size refers to the critical size
that separates the fine (elutriated) and coarse (remain
in bed) particles.
To ensure uniform and stable fluidization, the
type of distributor has to be chosen carefully. This is
to prevent poor fluidization quality of solids in certain
regions in the fluidized bed, to prevent plugging of
distributor-perforated holes, and to avoid solids from
dropping into windbox or gas plenum located be-
neath the fluidized bed. There are many types of
distributors available. Figure 8.3 (lower right image)
FIGURE 8.2 Various fluidization regimes exhibited by differshows four common types of distributors, namely,
ordinary (i), sandwiched (ii), bubble cap tuyere (iii),
and sparger (iv). It should be noted that pressure drop
Solids reservoir CycloneFeeder
Windbox
Gas fe
Heater Blower
FIGURE 8.3 Typical fluidized bed drying setup. Zones in a fluidupper right side image. Types of perforated distributor plates th
2006 by Taylor & Francis Group, LLC.across the distributor must be high enough to ensure
good and uniform fluidization.
As a rule of thumb, for upwardly and laterally
directed flow, pressure drop across the distributor
must exceed 30% of the pressure drop across the bed
[4]. Whereas for downwardly directed flow, the pres-
sure across the distributor must be greater than 10%
of the pressure drop across the bed. Upwardly direc-
ted flow is normally found in ordinary perforated
plates (Figure 8.3, lower right image-i). Sandwich-
type distributor is used if reinforcement of the
distributor is needed due to heavy load of bed of
classes of particles with increasing gas velocity.particles (Figure 8.3 lower right image-ii). Laterally
directed flow is normally obtained with bubble caps
and nozzle types of distributors (Figure 8.3, lower
(a) Freeboard; (b) dense phase
Solids hold up
ed Distributor plate
ized bed with its corresponding solids hold-up are shown in
at can be used are shown in lower right side image.
well as attrition-induced dusting.Spray drying, granulation, coating, and agglom-
eration share the same basic operating principle.
A fine spray of solutionpasteslurrysuspension isright image-i ii), whereas the sparger type gives lat-
erally or downward ly directed flow (Figur e 8.3,
lower right imag e-iv).
8.2 ADVANTAGES AND LIMITATIONSOF FLUIDIZED BED DRYERS
Commo nly recogni zed advan tages of fluidized bed
drying include: high rate of moisture remova l, high
therma l effici ency, easy mate rial trans port inside
dryer, ease of control , and low maintena nce cost.
Limitat ions of fluidized bed dryer include: high pres-
sure dro p, high electrica l power co nsumpt ion, poor
fluidiza tion qua lity of some particulat e pro ducts,
nonuni form product quality for certa in types of flu-
idized bed dryers , erosion of pipes an d vessel s, en-
trainment of fine pa rticles, attrit ion or pulveri zation
of particles , agglom eration of fine particles , etc. See
Mujumdar and Devahas tin [5] for detailed discus sion.
Bes ides drying, fluidized bed has found wide
ranges of ind ustrial ap plications in v arious indust ries
for mixi ng, de dustin g, granula tion, co ating, agglom -
eration , cooling , chemi cal react ions, incine ration ,
combust ion, gasific ation, etc. M any of these process es
can be incorpora ted with fluidized bed drying in one
unit process or to accompl ish two or more pro cesses in
the same unit. Processes that can be advan tageous ly
incorpora ted with fluidized bed drying a re de scribed
briefly in the followi ng pa ragraphs .
The mixi ng effec t in a fluidized be d is general ly
good for pa rticle sizes betwe en 50 and 2000 mm. Forfine particles (particl e size less than 50 mm), or forparticles that a re difficul t-to-flui dize when wet, vibra-
tion is nor mally app lied to impr ove the fluidiza tion
quality and the mixin g effe ct. For large particles ,
insertion of inter nals or use of the spouti ng mode
can help to improve the operation. For fluidized bed
drying, good particle mixing is essential. Thus, know-
ledge on particle fluidization characteristics and their
properties is required to ensure good performance of
a fluidized bed dryer. In addition, the bed of particles
can be fluidized by a pulsating flow or by fluidizing
sections of the bed periodically such that the entire
bed is fluidized in sequence once over a cycle. Clearly,
this operation results in saving of drying air and
hence electrical power but it also leads to a longer
operating time due to the intermittent mode of heat
input. Besides, intermittent fluidization can reduce
problem of mechanical damage to the particles due
to continuous vigorous particleparticle collision as 2006 by Taylor & Francis Group, LLC.atomized and sprayed in the fluidized bed of the
drying material itself or inert particles, which are
already loaded in the drying chamber. Formation
and growth of solid particles takes place in the cham-
ber as evaporation and drying carry away moisture.
In granulation, growth of solid particles is carried out
by successive wetting and coating of liquid feed onto
the solid particles, and solidification of the coated
layer by hot drying air. In coating, a layer of expen-
sive active agent can be coated on a less expensive
substrate, or to add a surface agent on solid particles,
which is needed for downstream processing. By spray-
ing a suitable binder onto the bed of solid particles,
agglomerated or granulated solid particles of large
particle size are produced.
In most cases, spray drying alone is not energy
efficient to remove all moisture content inside the
solids. This is because considerable amount of heat
and time is needed to remove internal moisture that
is trapped inside the solids internal. Fluidized bed
drying can be incorporated as the second-stage drying
to remove the internal moisture. This can be fol-
lowed by a third-stage fluidized bed cooling to avoid
the condensation problem during packaging in some
applications.
8.3 HEAT TRANSFER IN FLUIDIZED BEDS
Heat transfer in gas-fluidized bed can occur by con-
duction, convection, and radiation depending on the
operating conditions. The contribution of the respect-
ive modes of heat transfer to the coefficient of heat
transfer depends on particle classification, flow con-
dition, fluidization regimes, type of distributor, oper-
ating temperature, and pressure. Heat transfer
between a single particle and gas phase can be defined
by the conventional equation of heat transfer:
q hpAp(Tp Tg) (8:1)
where q is the rate of heat transfer (W), hp is the heat
transfer coefficient (W/(m2K)), Ap is the surface area
of a single particle (m2), Tp is the temperature of the
particle (K), and Tg is the temperature of gas (K).
The value of heat transfer coefficient of a single
particle in a fluidized bed system is generally not high.
It is in the range of 1 to 700 W/(m2K). However, due
to the large interfacial surface area, in the order of
3,000 to 45,000 m2/m3, extremely high rates of heat
transfer are achieved in this system. The heat capacity
is in the order of 106 J/(m3K). As a result, thermal
equilibrium is reached quickly. In designing fluidized
bed dryers, an isothermal condition is often assumed.
The heat transfer coefficient, hp, is a function of
the operating parameters, particulate characteristics,
and dr yer geomet ry. It can be estimat ed from the
followi ng co rrelatio ns dep ending on the parti cle
Reynol ds num ber, Rep :
hp kgdp
Nup (8 : 2)
where kg is the gas therm al condu ctivity (W/(m K)) ,
dp is the particle diame ter (m) , and Nu p is the parti cle
Nusse lt numbe r, and Prg is the gas Prand tl numb er [6].
For 0.1 Rep 50, Nu p 0.0282 Rep1.4 Prg0.33andfor 50 Rep 1 10 4, Nup 1.01 Rep0.48 Prg0.33Tubes, singl e or multiple , as well as fla t channels can
be immersed in a fluidized bed to provide addition al
heat for drying by condu ction. These surfa ces may be
vertical ly or horizont ally orient ed. Em pirical cor-
relations are available in the literat ure for v arious
geomet ries and operati ng conditio ns.
The surfa ce-to-bed heat transfer coeffici ent,
hw q/ aw (T b T w ), is based on the surface a rea ofthe submer ged object . Thi s coe fficient consis ts of two
compon ents, convecti ve and radiative if the tempe ra-
ture is high . Here aw is wall surface area (m2) and TW
is wall tempe rature (K) , Tb is bed tempe ratur e (K).
The convecti ve he at trans fer coeffici ent, hc , can be
estimat ed us ing correl ation by Vreed enberg [7] for
horizont al imm ersed obj ects:
hc dt
kg 420 rs
rgPrg
m 2g
gr 2s d 3p
!0 :3Re0 :3t if
rsrgRep 2550
(8 : 3)
hc dt
kg 0:66 Pr 0: 3g
rs (1 )rg
!0 :44Re 0: 44t if
rsrgRep 2050
(8 : 4)
In these eq uations, dt is the column diameter (m) , rs isthe particle den sity (kg/m 3), rg is the gravi tation alaccele ration (m/s 2), mg is the g as viscos ity (Ns /m
2),
is the void fraction, and Re is the Reynold s numb erdefined by
Ret dt r g ug
mg(8 : 5)
and
Rep dp r g ug
mg(8 : 6) 2006 by Taylor & Francis Group, LLC.The radiant heat transfer coefficient, hr (W /m2 K) ca n be
estim ate d u sing the following e quation among o the rs [8 ]:
hr eb e web e w e b e w
s ( T 4b T 4w )( Tb Tw ) (8 : 7)
where s is the StefanBoltzmann constant. Radiativeheat transfer is insignificant at temperatures, T, lower
than 7008C. Typically bed emissivity, b, is approxi-mately 0.9 and wall emissivity, w, is between 0.9 and1.125 [8]. Since most drying processes are carried out
at temperatures lower than 7008C, radiant heat trans-fer can be neglected.
The effect of various operating parameters on the
heat trans fer co efficient is given in Tabl e 8.2.
8.4 MATHEMATICAL MODELSOF FLUIDIZED BED DRYING
Many mathematical models of fluidized bed drying
have been proposed in the literature and verified with
experimental data. These models have been developed
based on different assumptions.
8.4.1 DIFFUSION MODEL
This model assumes that drying of single particles in a
fluidized bed is totally controlled by diffusion of
moisture inside the particle. For the analysis of par-
ticulate drying, diffusion equation for spheres of an
equivalent diameter can be used. Zahed and Epstein
[23] developed a diffusion model for spout bed drying
and later Martinez-Vera et al. [24] applied the same
model for fluidized bed drying.
This model assumes
. Solids are spherical, isotropic, uniform size, and
homogeneous. They are perfectly well mixed in
fluidized bed.. Physical properties of the dry solids remain
constant with time.. Solids shrinkage and temperature gradient in-
side the solid are negligible.. Drying kinetics is governed by internal moisture
diffusion. Thus, moisture at the solid surface is
in equilibrium with the bed air humidity.. Air is perfectly mixed. Exhaust air is in thermal
equilibrium with bed.. The dryer is perfectly insulated.
The diffusivity is assumed constant. The following
diffusion equation defines moisture transport:
@X
@t D @
2X
@r2
2r
@X
@r
(8:8)
sfe
ea
; fo
oth
num
xim
d de
g
loc
ith
re
r sm
vec
incTABLE 8.2Effect of Operating Parameters on Particle Heat Tran
Parameter Effect on H
Particle
Diameter, dp For fine particles, h is higher
Shape Higher for rounded and smo
Specific heat, cp h /cpn, where 0.25 < n < 0.8Thermal conductivity, kp No influence for small Biot
Gas
Velocity, ug Increases above umf to a ma
optimum velocity, uopt an
Density, rg Increases with increasing, rgViscosity, mg Increases with decreasing, m
Specific heat, cg At moderate pressure and ve
At high pressure, increases w
Thermal conductivity, kg h / kgn, where 0.5 < n < 0.66h Increases as bed temperatu
Fluidized bed
Bed height, Hb No influence
Bed diameter, db No information available
Bed temperature, Tb Gas-convective: increases fo
Bed pressure, Pb No influence on particle-con
Gas-convective heat transfer
Heat transfer surfacewhere X is the free mois ture content , i.e., that in
excess of the equilib rium value, D is the diffusiv ity
(m2/s), and r is radial dimens ion (m).
If diffusiv ity is varia ble and depend ent on the
radial dist ance of drying bounda ry from the center
of the so lids, the foll owing diffusion equatio n is used
instead :
@ X
@ t D @
2 X
@ r 2
2r
@ X
@ r
@ D@ X
@ X
@ r
2(8 : 9)
Once the diffu sivity is know n, numerica l an alysis is
applie d to the diffusion eq uation in order to find
moisture content pro file insid e the so lid. Dif fusivity
of various food products can be obtaine d from
Sablani et al. [25] . Average moisture con tent,X , can
be obtaine d from the followin g eq uation:
X 4pVp
rp0
r2 X d r (8 : 10)
where Vp is the parti cle volume (m 3). Note that mois -
ture content and temperatur e-depen dent diffusiv ity
values can be used to solve the equati on num erically.
Length, L No influence
Tube diameter, dtube Increases with decreasing dtube
2006 by Taylor & Francis Group, LLC.r Coefficient
t Transfer Coefficient, h Reference
r coarse particles, h is lower 9
surface particles 10,11
12,13
ber 14,15
um value at an
creases thereafter
9
10,11
ity, no information available 16,17
increasing cg
14,18
increases, due to increasing of kg
12,19
all particles; decreases for coarse particles 20
tive heat transfer 21
reases8.4.2 E MPIRICAL MODEL
In this model, the drying pro cess is divided into dif-
ferent periods wher e drying mechani sms in each dry-
ing pe riod are different .
The general solution of Fick s diffu sion express es
the mois ture content in terms of the drying time in
exponen tial functi on. The solut ion for spheri cal solid s
is given in the folowing the eq uation [2628 ]:
Sphere:
X XeqXo Xeq
6
p 2
X1n 1
1
n2 e n2 (p2 D eff t= r 2sph ) (8 : 11)
where rsph is the sphere radius (m), Deff i s t he e ff ec ti ve
di ff us iv it y ( m2/s ) a nd L is slab half thickness. Subscript
eq denotes equilibrium and o indicates initial state.
Since the general solution of the diffusion equa-
tion is expressed as a series of exponential functions,
experimental data obtained from fluidized bed drying
can be correlated as an exponential function. Many
empirical exponential equations have been proposed.
Equat ion 8.12 is a simp le exponenti al equati on. It
assumes that the drying rate is proportional to the
22
17
difference between the average mois ture content and
the eq uilibrium mo isture content [29] :
X XeqXind X eq e
kt (8 : 12)
where subscri pt in d denotes inductio n pe riod.
Equation 8.13 is a modified version of Equation
8.12 by Henders on and Pabi s [30] . This equ ation is
also an alogous to the theoret ical diffusion equ ation
solution for an infin ite slab [26,31]. Com paring Equa-
tion 8.13 and Equation 8.11, b Deff p2/r 2sph [32]:
X XeqXind X eq ae
bt (8 : 13)
Equation 8.12 tends to overpredi ct the early stage and
underp redict the late r stage of drying. Equation 8.14
is an empirical modificat ion of Equation 8.12 by
introd ucing an expo nent y [33]. It ha s been used
most commonl y because most exp erimental data can
be fitted very well with the follo wing equati on:
X XeqXind Xeq e
xt y (8 : 14)
Equation 8.15 uses the first two term s from Fi cks
second law of diff usion. This eq uation has be en used
regardl ess of solids geomet ry [34] :
X XeqXind Xeq a1 e
b 1 t a2 e b2 t (8 : 15)
It should be noted that drying constant s in the models
mentio ned ab ove are empirical and dep end on the
type of material s, ope rating co ndition s as wel l as
dryer dimens ions. If one of these models is used for
fluidized be d dryer design, experi mental invest igation
on drying kineti cs has to be condu cted to obt ain the
drying constant for the particu lar mate rial prior to
the dr yer design.
8.4.3 K INETIC MODEL
Chandr an et al. [35] developed a kin etic model for
fluidized be d drying of solid s. For a batch fluidized
bed kinetic model, it is assum ed that the drying pr o-
cess ha s bot h constant and falling rate pe riods. Dry-
ing rate in the falling rate period falls linearly wi th
decreas ing mois ture content . Feed conditio ns and
total contact area betwee n soli ds and hot a irstream
remain the same throughou t the whol e drying pr o-
cess. In the batch drying operation, there is little
interaction between the particles (wet and dry par-
ticles) in the system. Thus, data on drying kinetics is 2006 by Taylor & Francis Group, LLC.sufficient to estimate the residence time of solids in
order to achieve the desirable final moisture content.
Moisture content of solids in different drying periods
can be estimated from the following equations.
In the constant rate period,
X Xo at (8:16)
In the falling rate period,
X Xeq (Xcr1 Xeq)ea(ttcr1)=(Xcr1Xeq) (8:17)
where subscript cr1 denotes the first critical point
that distinguishes constant and falling rate periods.
For a single-stage continuous fluidized bed kinetics
model, solids exit the fluidized bed system with a
distribution of moisture content due to the wide
residence time distribution. An average value of the
moisture content and residence time is used.
The average moisture content of solids in a con-
tinuous fluidized bed drying is given by
X
Xo
X
Xo
b
E(u) du (8:18)
where (X/Xo)b is the moisture ratio in batch fluidized
bed dryer, E(u) is the residence time density for thesolids, and E(u) eu. u t/tcr1 is dimensionlesstime. Subscript b denotes batch process [36].
In the constant rate period,
X
Xo 1 att
Xo(8:19)
In the falling rate period,
X
Xo 1 att
(bt 1)Xo (8:20)
For a continuous fluidized bed that exhibits both
constant and falling rate periods, the moisture content
is then given by the following equation:
X
Xo 1 att
Xo
btte ucbtt 1 1
(8:21)
where b a/(Xcr1 Xeq), uc t/tcr1,X is the averagemoisture content, tt is the average residence time, anda is the drying coefficient.
Once the average moisture content is known,
equations obtained from mass and energy balances
in the following models can be used to calculate the
humidity and temperature of the exhaust air as well as
the solids temperature. The simplest model is the
single-phase model that treats the fluidized bed as a
continuum. As the number of phases considered in
the model goes higher, the fluidized bed drying model
becomes more complex and involves more transport
properties. Complicated fluidized bed drying models
that account for many transport processes that occur
within and across the phases are beyond the scope of
this chapter.
8.4.4 SINGLE-PHASE MODEL
In a single-phase model, the fluidized bed is regarded
essentially as a continuum (Figure 8.4). Heat and
mass balances are applied over the fluidized bed. It
is assumed that particles in the bed are perfectly
mixed. Equation 8.22 and Equation 8.23 are the
equations of moisture balance and energy balance,
respectively [24].
Moisture Balance:
Ms dXdt Gg(Yout Yin) (8:22)
where cp is the heat capacity at constant pressure (kJ/
(kg K)) and l is the latent heat of vaporization(kJ/kg). Subscript s denotes wet solid, g denotes
dry air, and v denotes water vapor. Equation 8.23
neglects sensible heat of the water in solids.
8.4.5 TWO-PHASE MODEL
A simple two-phase model of fluidized bed drying
treats the fluidized bed to be composed of a bubble
phase (dilute phase) and an emulsion phase (dense
phase). The bubble phase contains no particles or
the particles are widely dispersed. This model assumes
that all gas in excess of minimum fluidization velocity,
umf, flows through the bed as bubbles whereas the
emulsion phase stays stagnant at the minimum fluid-
ization conditions [37]. Figure 8.5 shows a schematic
diagram of the simple two-phase model.
Zahed et al. [38] have presented mass and energy
balance equations for the dense phase and the bubblewhereMs is the mass hold-up of dry solid in bed (kg),
X is the average moisture content (kg/kg), Gg is the
mass flow rate of dry air (kg/s), and Y is the air
humidity (kg(water vapor)/kg(dry air)).
Energy Balance:
MscpsdT
dt Gg(cg Yincv)(Tin Tout) Gg(Yout Yin)l (8:23)
Inlet drying airYin, Tin, Gg
Outlet drying airYout, Tout
Solid particlesms, Ts, cs
FIGURE 8.4 Schematic diagram of the single-phase modelof fluidized bed dryer. 2006 by Taylor & Francis Group, LLC.phase for fluidized bed drying. Mass balance of liquid
in the bubble phase gives the following equation:
rgbbdYbb
dt rg
VgbbVbt
(Ybb Yin)
6Kcrgbbdbb
(Yd Ybb) (8:24)
where subscript bb denotes bubble phase and d
denotes dense phase. The rate of change of mass in
the bubble phase can be assumed to be negligible [38]
and Equation 8.24 can be rearranged to express hu-
midity in the bubble phase, Ybb in terms of humidity
in the dense phase, Yd. In the equation, Vgbb/Vb is thegas flow rate in bubble phase per unit volume of bed.
Dense phaseparticulate solids
Dilute phasebubbles
Gas crossflow
Gas flow
FIGURE 8.5 Schematic diagram of a two-phase model forfluidized bed drying.
face moisture. Increasing the gas velocity increasesKc is the mass transfer coeffici ent across the bubble
bounda ry.
M ass balance of liquid in the interstiti al gas in the
dense phase gives the followi ng equatio n:
6Kc r g bb
dbb( Ybb Y d ) r g
Vg dVb t
( Yd Y in ) _mm
rg mf (1 bb )DYd
dt (8 : 25)
Likew ise, the rate of change of mass in the interstiti al
gas can be assum ed to be negligible . In this equatio n,
_mm is the mass rate of evap oration of wat er per unitvolume of bed, which in turn can be obtaine d from
mass balance on de nse phase. Vg d /V b is the gas flowrate in dense phase per unit volume of bed.
M ass ba lance of liquid in the dense-phas e pa rticles
yields the followin g eq uation:
_mm rp (1 mf )(1 bb )dX
dt(8 : 26)
The coupled mass and energy balance in dense pha se
that consis ts of parti cles and interstiti al gas pha ses is
given in the followin g eq uation:
rp (1 mf )(1 bb )(c ps c plX )dTp
d t
rgVg dVb t
( c pg Y in c pv )( Tg in Tp ) DH evap
rgVg dVb t
( Yd Yin ) 6Kc r g bb
dbb( Ybb Y d )
(8 : 27)
The above equa tion express es the change of parti cle
tempe rature in the dense phase in terms of average
moisture content , X , whi ch can be determ ined from
any one equ ation from Equation 8.8 through Equa-
tion 8.21 depen ding on the ope rating con ditions and
the drying model, humidi ty of dense and bubble
phases, Yd , Y bb, en thalpy of evaporat ion, DH evap ,bubble diame ter, dbb , and mass transfer co efficien t
of bubble bounda ry. Solving Equat ion 8.27 yield s
the so lids temperatur e at diff erent drying times.
8.5 EFFECT OF OPERATING PARAMETERSON FLUIDIZED BED DRYING
8.5.1 E FFECT OF B ED HEIGHT
For mate rials wi th high mobil ity of inter nal mois ture
such a s iron ore, ion-ex chan ge resin s, silica gel, most
drying takes place close to the dist ributo r plate . Bed
height has no effect on its drying rate that increasing 2006 by Taylor & Francis Group, LLC.the drying rate. However, gas velocity has no effect
at all for particles with high internal resistance to
moisture transfer. High internal moisture resistance
dominates at the end of the falling rate period.
8.5.4 EFFECT OF BED TEMPERATURE
Bed temperature is increased by high external heat
fluxes. This in turn leads to higher moisture diffusiv-
ities and hence higher drying rate. This effect is com-
plex and depends on the relative significance of
external and internal resistances to moisture transfer.
8.6 TYPES OF FLUIDIZED BED DRYERS:CLASSIFICATION AND SELECTION
Various types of fluidized bed dryers have been studied,
developed, and operated in many industrial processes
according to the respective process, product, oper-
ational safety, and environmental requirements. It is
important to become familiar with the specific charac-
teristics of different fluidized bed types in order tomake
a logical and cost-effective selection. It should be noted
that in many instances several different types may pro-
vide similar performance at the same cost.
Some novel fluidized bed dryers, which have not
found application in industrial drying, are used to
overcome disadvantages and difficulties that may
occur in conventional fluidized bed dryers. It should
be noted that not all modified fluidized bed dryers
are necessarily better than the conventional dryers
in terms of product quality, or energy efficiency, or
drying performance.bed height beyond a particular value leads to no
differences in drying rates. For materials with main
resistance to drying within the material, e.g., grains,
drying rate decreases with increasing bed height.
8.5.2 EFFECT OF PARTICLE SIZE
For group B particles (sandlike particles, according
to Geldart Classification of Powdes), drying time that
is required to remove a given amount of moisture
increases as the square of the particle diameter pro-
vided that all other conditions remain unchanged.
However, this effect is much smaller for group A
(aertable particles, according to Geldart Classifica-
tion of Powdes) particles because these particles are
finer than group B and it exhibits smooth fluidization
before entering bubbling fluidization regime.
8.5.3 EFFECT OF GAS VELOCITY
Gas velocity has a dominant effect on removing sur-
TABLE 8.3Classification of Fluidized Bed Dryers
Criterion Type of Dryer Subclassification
Processing mode/feed
and discharge
. Batch FBDs (well-mixed)
. Semicontinuous FBDs
. Continuous . Well-mixed FBDs. Plug flow FBDs or. Single stage. Multistage FBDs. Hybrid/combined FBDs
Particulate flow regime . Well-mixed FBDs. Plug flow FBDs. Circulating FBDs. Hybrid . Multistage FBDs (well-mixedplug flow)
. Hybrid/combined FBDs
Operating pressure . Low (for heat-sensitive products,
low pressure strategy). Near atmospheric (most common). High (5 bars, superheated steam FBDs)
Fluidization gas flow . Continuous. Pulsed FBDs
Fluidizing gas temperature . Constant. Time-dependent . Step down
. Step up
. Periodic (zigzag)
. Combined
Heat supply . Convective. Convective/conduction (immersed FBDs)
or
. Continuous
. Intermittent (multiple variable strategy)
Fluidization action . By gas flow (pneumatic) . Ordinary FBDs. Circulating FBDs
. By jet flow . Spouted FBDs. Recirculating FBDs. Jetting FBDs
. With mechanical assistance . Vibration (vibrated FBDs)
. With external field . Agitation (agitated FBDs). Rotation (centrifugal FBDs). Microwaveradio frequency field (MWRF FBDs). Acoustic field. Magnetic field
Fluidized material . Particulate solid (most common) . Group A and B (most common, conventional FBDs). Group C (vibrated FBDs, agitated FBDs). Group D (vibrated FBDs, baffled FBDs, spouted FBDs)
. Paste/slurry . Spray onto a bed of inert particles (inert solids FBDs). Spray onto absorbent particles (silica gel, biomass). Spouted FBDs
Fluidizing medium . Heated air/flue gases/direct combustion gas. Superheated steam/vapor. Dehumidified cool air (heat pump FBDs). Air below freezing point of liquid being
removed (fluidized bed freeze dryers)
2006 by Taylor & Francis Group, LLC.
Tabl e 8.3 class ifies the divers e varia nts of fluid ized
bed dryers according to various criteria.
8.7 CONVENTIONAL FLUIDIZEDBED DRYERS
8.7.1 BATCH FLUIDIZED BED DRYERS
A batch fluidized bed dryer is used when production
capacity required is small (normally 50 to 1000 kg/h)
or several products are to be produced in the same
production line. It is preferable to operate batchwise
if upstream and downstream processes are operated
in batch mode, or several processes are to be carried
out in sequence (e.g., mixing, drying, granulation/
coating, cooling) in the same processing unit.
Drying air temperature and flow rate are normally
tinuous fluidized bed dryer where the batches are
rotated. In addition, gas temperature and velocity at
different batches can be varied.
8.7.3 WELL-MIXED, CONTINUOUS FLUIDIZED
bed
Rotation Wet solids
Exhaustair
Dry solids
Heated air
FIGURE 8.7 Semicontinuous fluidized bed dryer.
lot air orflue gasDry solids
Wet solids
FIGURE 8.8 Well-mixed fluidized bed dryers.FIGURE 8.6 Batch fluidized bed dryer.fixed at a constant value. However, by adjusting the
airflow rate and its temperature, it is possible to save
energy and reduce attrition. Mechanical assistance
such as agitation or vibration is normally applied
for processing materials that are difficult-to-fluidize.
Figure 8.6 shows a typical batch fluidized bed dryer
with expanded freeboard and built-in internal bag fil-
ters. Expanded freeboard is used to reduce elutriation
of fine particles.
8.7.2 SEMICONTINUOUS FLUIDIZED BED DRYERS
In semicontinuous fluidized bed drying system, the
drying chamber consists of a series of subprocessors.
The wet product is accurately dosed and charged into
the batches. The product is either transported batch-
wise from one processor to another processor or the
batches (the processors with the batches of product)
rotates along the process line [39]. This gives uninter-
rupted continuous operation over a long period.
Figure 8.7 shows a schematic diagram of a semicon-
Bagfilters
Fluidized 2006 by Taylor & Francis Group, LLC.BED DRYERS
The well-mixed continuous fluidized bed dryer
(Figure 8.8) is one of the most common fluidized
bed dryers used in the industry. As the bed of particles
is perfectly mixed, the bed temperature is uniform and
is equal to the product and exhaust gas temperatures.
However, particle residence time distribution is neces-
sarily wide, thus resulting in wide range of product
moisture content. On the other hand, as the feed
material is continuously charged into the fluidized
bed of relatively dry particles, this gives the added
advantage of enhanced fluidizability and better fluid-
ization quality. In some cases, a series of well-mixed
continuous dryers may be used with variable operat-
ing parameters. In addition, a well-mixed continuous
Exhaust air
fluidized bed dryer can be incorpora ted with othe r
types of dryers su ch as plug flow fluidized be d dryers
to give bette r drying perfor mance.
8.7.4 P LUG FLOW F LUIDIZED BED DRYERS
In plug flow fluidized be d dryers , verti cal ba ffles are
inserted to create a narrow pa rticle flow path, thu s
giving relative ly narrow parti cle residen ce time distri-
bution. Particles flow co ntinuous ly a s a plug from the
inlet toward the outlet through the path. This en sures
nearly equ al residen ce time for all particles irre s-
pective of their size and ensures unifor m produ ct
moisture content . Various paths can be de signed such
as straight or spiral paths. Length-to -width ratio is
two or more process es can be carri ed out a nd accom-
plished in a fluid ized bed column. Thi s can be
achieve d by sim ply ch anging the operati ng co ndition s
of fluidized bed to mix, dry, gran ulate, or coat [40] , or
cool in a singl e unit without dischar ging the material
from the unit.
In a fluidized bed spray dryer, spray drying is
carried out in the upper part of the ch amber fol-
lowed by fluidized bed drying or agglom erati on (Fig-
ure 8.10a). The large -scale fluidized bed coal dryer is
also a particle class ifier (Figure 8.10b). Dryi ng and
classificat ion (separati on of fine s) are ca rried out in
the same fluid ized bed. By chan ging the fluidizi ng g as
velocity, cut size (part icle size that separat es fine and
coarse particles ) can be adjust ed in the class ification
Ex
D
; (Various types of modified fluidized bed dryers have
been developed an d ap plied in many indust rial pr o-
cesses. M odified fluidized bed dryers are app lied to
overcome some of the prob lems and disadva ntages
encoun tered in conven tional fluidized beds.
8.8.1 MULTISTAGE AND MULTIPROCESS FLUIDIZEDB ED DRYERS
As fluidized beds offer many dist inct features and
advantag es for process ing of parti culate mate rials,
(a)
Exhaust gas Wet solid
Hot air
Perforateddistributor
Dry solid
FIGURE 8.9 Plug flow fluidized bed dryers. (a) Straight pathnormal ly in the range of 5:1 to 30:1. Figu re 8.9
shows a plug flow fluidized be d dr yer of stra ight and
reverse paths.
Opera tional problem s might occu r at the feed inlet
because wet feedsto ck must be fluidized direct ly ra-
ther than when mixe d with drier mate rial as in the
case of a well-mixe d unit. To ov ercome the pr oblem of
fluidiza bility at the feed inlet , the inlet region may be
agitated with an agitator, or by applying backmixing of
solids, or by using a flash dryer to remove the surface
moisture prior to plug flow fluidized bed drying.
8.8 MODIFIED FLUIDIZED BED DRYERS 2006 by Taylor & Francis Group, LLC.process . Anothe r examp le is upper stage of fluidized
bed drying that can be follo wed by a low er stage
of fluidized bed cooling (Figure 8.11a). A fluidized
bed dryer or cooler consists of first-stage fluidized bed
dryer followed by second-stage fluidized bed cooling
(Figure 8.11b).
In add ition, diff erent types of fluidized bed sys-
tems can be incorpo rated in a process ing uni t as well.
For inst ance, first-st age well- mixed fluidized bed pre-
drying can be incorpora ted with second-s tage plug
flow fluidized be d drying (Figur e 8.11a) . By inco rpor-
ating different process es an d co mbinin g diffe rent
types of fluid ized beds, sp ace requir ement , install a-
tion costs, an d energy co nsumpt ion can be reduced
appreci ably.
8.8.2 HYBRID F LUIDIZED BED DRYERS
Hybrid fluidized bed dryers are useful for through
drying of solids that con tain surface and intern al
moistures . Surface mois ture can be remove d in the
first-st age drying using a flash or cyclone dryers . Se c-
ond-stage drying is then carried out in fluidized
bed dryers in which residence time can be easily
control led. Figure 8.12 sh ows an exampl e of hyb rid
(b)
Perforateddistributor
haust gas Wet solid
Hot air
ry solid
Partition plate/ internal baffle
b) reversing path.
cyclone fluidized bed dryer [39]. Wet solids are first It was foun d that the roto- fluidized dryer perfor ms
(a) (b)
Exhaust gas
Liquid
Hot gasDry solids
Solidsinlet
Exhaust gas
Fluidized bedcoal dryer
Solids outlet
Heated air
FIGURE 8.10 (a) Spray fluidized bed dryer; (b) fluidized bed coal dryer and classifier.charged into the cyclone dryer by exiting flui dizing
gas from fluidized bed dryer. Surface mois ture
content of soli ds is quickly remove d with the gas
in the c yclone dryer. Solids and gas are separat ed in
the cyclone. Par tially dried soli ds are then pne uma-
tically co nveyed into the fluidized bed for second -
stage drying. Othe r types of hybrid fluidized bed
dryers include flash-flui dized bed dryer, filter-flu idized
bed dryer [41] .
A mult istage spray fluidized bed dryer con sists of
a spray chamb er followe d by first- stage fluidized bed
drying a nd second-s tage fluidized bed coo ling (Fig-
ure 8.13). When soli d powder s a re form ed in the sp ray
dryer, these powder s still con tain some intern al mois -
ture. It is costl y to use a spray dryer to remove all of
the inter nal mois ture. Instead, using a second-s tage
fluidized bed dryer is mo re co st-effecti ve. Lisbo a et al.
[42] applie d fluidiza tion techniq ue in a con ventio nal
rotary. The dryer is known as roto- fluidized dryer.(a)
Product Heated air
Lowerstage
Upperstage
Inlet solids
Wet solid
Exhaust air
FIGURE 8.11 Two-stage fluidized bed dryers. (a) Upper stagefluidized bed; (b) first-stage dryer followed second-stage cooler.
2006 by Taylor & Francis Group, LLC.better than the co nventi onal rotar y dryer.
8.8.3 P ULSATING F LUIDIZED BED DRYE RS
Pulsating fluidized bed dryers are used to overcome the
problems of restricted particle size and size distribu-
tion, as well as aggregative fluidization and channeling
that occur in a conventional fluidized bed dryer when
processing certain types of powders. By pulsating the
fluidizing gas stream, the fluidized bed either the whole
bed or part of the bed is subjected to variable fluidizing
gas velocity (Figure 8.14) [4346]. This contributes to
effective energy costs saving and enhanced drying per-
formance without affecting the fluidization quality and
process performance or added extra capital costs. For
larger particles (group D particles), intermittent spout-
ing of the bed with a rotating spouting jet has been
shown to reduce energy consumption with only a mar-
ginal increase in drying time for batch drying.(b)Hot air
sExhaust air
Cooling air Cooling air
Exhaust air
well-mixed fluidized bed followed by lower stage plug flow
increa ses the co ntacting efficien cy betw een the bed
and the he at trans fer surface. However, heat trans fer
coeffici ent reaches a maxi mum value. Bey ond this
point, increa sing superfici al gas veloci ty will hind er
heat transfer betw een the bed and the heati ng surfa ce.
This is be cause of increa sing prepon derance of bubble
(not pa rticles ) at the heatin g surface, which de crease s
particle- to-wal l heat transfer.
8.8.5 MECHANICALLY ASSISTED FLUIDIZEDB ED DRYERS
Fluidi zation quality of fine and large pa rticles can be
enhance d by the assistanc e of extern al means such as
vibration or agitati on. Mo reover, these pa rticles can
be imm ersed in a bed of fluidiza ble inert pa rticles to
impro ve their fluidiza tion qua lity [47] .
Wetsolid Exhaustgas
Cyclonedryer
Fluidizedbed dryer
Pneumaticconveyor Air
Drysolid Hot gas
FIGURE 8.12 Hybrid cyclone fluidized bed dryer.8.8.4 F LUIDIZED BED DRYERS WITH IMMERSEDHEAT EXCHANGERS
Fluidi zed beds equipped with inter nal heater s or im-
mersed tubes transfer he at indire ctly to the drying
material . Hori zontal tube bundl es (Figur e 8.15) are
used extens ively compared to vertical type. Tube
pitch is an important design parame ter. Fluidizing
gas stream fluidizes the material and carries over the
evaporat ed moisture. As a resul t, total sensible he at
of gas and thus qua ntity of ga s require d are redu ced.
Immersed tubes or intern ally heated fluidized bed
dryers are use d to dr y smaller size or fine powder s.
This is because he at trans fer coefficie nt decreas es wi th
increa sing pa rticle size. Inste ad of tubes, verti cal
plates are also used as immersed heater s.
Heat transfer is highly dep endent on the parti cle
heat capacity an d mixing. Vigorous bubbl e action
gives bette r pa rticle circul ation an d mixi ng, an d thu sFeedLiquid
Heated airAglomerationchamber
Vibro-fluidi
CooHeated air
Recycled fine, crushed coarse
FIGURE 8.13 Multistage fluidized bed spray dryer.
2006 by Taylor & Francis Group, LLC.8.8.6 V IBRATED FLUIDIZED B ED DRYERS
Vibratio n co mbined wi th upwar d flow of air in an
aerated bed enables particles to pseudofl uidize
smoot hly. The gas velocity requ ired for minimum
fluidiza tion is consider ably lower than the mini -
mum fluidiza tion veloci ty in conventi onal fluidized
bed dryer. Attri tion due to vigorou s acti ons between
particlepa rti cle and pa rticlewal l is thus mini mized
appreci ably. Hence, application of fluid ized bed can
be extende d to fragile, abrasi ve, and heat-sensi tive
material s. The problem of fine particle entrain ment
is also avoided. For pol ydisperse powder s, low g as
velocity fluid izes the fine particles gentl y wherea s
vibration keeps the coarse parti cles in a mobil e stat e.
Vi brating fluidized beds are gen erally plug flow
type (Figur e 8.16). Vi brating fluidized beds are rela-
tively shallow as the effect of vibration imparted by
the vibrating grid decays with distance from the grid.
Exhaust gas Exhaust gas
zer
Cyclone
Particles
Sieve
FineCoarseDesirableproduct
l air
Wetfeed
I
Hot air
FIGURE 8.14 Pulsating fluidized bed. Parts of the bed are fluidThere are some acoustic noise issue s associ ated wi th
such devices . Thes e units can ope rate in batch as well
as co ntinuous modes.
8.8.7 A GITATED FLUIDIZED B ED DRYERS /SWIRLF LUIDIZERS
Anothe r way to impr ove fluidiza tion quality of fine
particles is to impar t mechani cal agit ation to the bed
(Figur e 8.17) . By agit ation, a hom ogeneou s fluidizedExhaust gas
Solidsinlet
Solids flow
Gas flow
Immersed tube
Hot gasSolids out
Heatingfluid
FIGURE 8.15 Immersed tubes fluidized bed dryer.
2006 by Taylor & Francis Group, LLC.bed is form ed withou t chan neling or form ation of
large bubbles. Mo reover, agitated fluid ized bed dryers
are useful for drying pastes or cakes con sisting of fine
particles [48] . In this case, agit ation helps to disi nte-
grate an d disperse the pasty feed. The agitator serves
as a mixer in the dryer [49]. Moreover, deeper bed
depth is possibl e if the bed is ag itated wher eas its
fluidiza tion qua lity is maintained.
8.8.8 F LUIDIZED BED DRYERS OF INERT P ARTICLES
Exhaust air
Product
Perforateddistributor
nlet gas distributor
ized periodically.In recent years, the app lication of fluidized bed drying
has be en extended to drying of fine powder s, pastes ,
slurries, suspen sions, pulp, an d enzymes -containing
aqueou s med ium [5055 ]. Thi s is accompl ished by
using inert pa rticles of high he at capacit y (Figur e
8.18) [56] . Inert pa rticles must be able to fluidize
well in a fluidized bed . By mixi ng the inert pa rticles
whose fluidiza tion qua lity is gen erally good wi th the
material s men tioned ab ove, the fluid ization qua lity of
the mate rials is impr oved ap preciab ly [57,58]. In ad d-
ition, the inert particles with high heat ca pacity serve
as energy carriers that enhance he at trans fer [59,60].
Drying on inert particles can be performed in a var-
iety of fluidized be ds namel y ordinar y fluidized bed ,
spouted bed, spouted fluidized bed , jetting- spouted
bed, as well as v ibrated fluidized bed [61].
The liquid to be dried is sprayed into the fluidized
bed; it coats the inert particle surfaces. The coated
layer dries as a result of combined convective heat
transfer from hot air and contact heat transfer due to
sensible heat of the particles. When the thin layer is
dry, it becomes brittle , cracks, and is pe eled off
due to attrit ion by particlepa rticle an d parti clewal l
collisions . As a resul t, a fine powder is formed and is
carried over by the exh aust gas to be collected
and separat ed in suitable gas-c leaning de vices such
transp orts the parti cles to the bed surfa ce. Ener getic
spouti ng at the be d surfa ce thrust s the parti cles
into the freeboa rd region at the center of the bed
(Figur e 8.19) . After losi ng their momen tum, these
Exhaust air Flexiblecouplings
Wet solids
Dry solids Hot air
Vibrator
FIGURE 8.16 Vibrating fluidized bed.as cyc lones or bag filters.
8.8.9 S POUTED B ED DRYERS
Spouted be d dryers are useful for drying of large
(Geldart s group D) pa rticles ( >5 mm), which exhibi tsluggin g unde r nor mal fluidiza tion. In a spo uted be d,
a high gas veloci ty jet of gas pe netrates throu gh an
opening at the bottom of the bed of parti cles and
Exhaustair
Solids inletRotation
Agitator
Heated air
Product
FIGURE 8.17 An agitated fluidized bed dryer.
2006 by Taylor & Francis Group, LLC.particles fall back onto the bed surfa ce. Thr ough
this fountain-l ike acti on, good solid mixin g is in-
duced. A cyc lical flow of particles is thus created .
Details of spou ted bed dr ying are discus sed elsewh ere
in this handbo ok.
The spout bed has be en applie d to drying, gran u-
lation, co ating as well as to dr ying of pastes , solu-
tions, slurr ies, and su spensio ns. M ujumdar [62] ha s
classified spouted beds into at least 30 different vari-
ants, each with a specific set of advantages and limi-
tations. Periodically spouted beds, multiple spouted
Exhaust gasLiquid
Fluidizing gas
FIGURE 8.18 Inert solids fluidized bed.
Bed surface
Spoutbeds, two -dimensiona l sp outed be ds, and oscillat ing
spouted be ds are some of the ideas introd uced by
Mujumdar in 1985, which have been examin ed in
the lite rature in recent years.
8.8.10 RECIRCULATING FLUIDIZED B ED DRYERS
Insertion of a tubular draft tube into an ordinar y
spouted fluidized bed changes its ope ration al and
design characteris tics. This type of fluidized bed is
known as recircu lating fluidized bed (or inter nally
circulati ng fluid ized bed, see Figure 8.20) . Unlike
spouted beds, recir culating fluidized beds do not
have limitation of maxi mum spoutabl e be d height
and minimum spouti ng veloci ty. As spouti ng gas
stream passes throu gh the draft tub e, it is co nfined
within the tube and does not leak out horizont ally
toward the downcom er. After passin g throug h the
draft tube, particles foll ow a certa in flow patte rn in
the be d and flow down ward in downcom er region.
Sinc e there is more flexibility in ope rating recir cu-
lating fluidized bed , it is applic able to ha ndle all
Conicalbase
Spouting gas
FIGURE 8.19 Spouted bed dryers.
2006 by Taylor & Francis Group, LLC.groups of powder s and particles . Its a pplication in
drying has been repo rted in co ating of table ts in
pharmac eutic al indust ries, and in drying of dilute
solutions co ntaining soli ds. How ever, it is not a
Exhaust gas
Draft tube Solids outDowncomer
Solids flow
Gas flow
Gas andsolid feed
FIGURE 8.20 Recirculating fluidized bed dryer.common dryer type now.
8.8.11 JETTING FLUIDIZED B ED DRYERS
In an ord inary flui dized bed, inlet gas is passed
through noz zles, which are perfora ted e venly across
the distribut or plate . Jett ing regions appea r above
every nozzle. In a spouted bed , inlet gas stre am is
suppli ed through a cen trally located jet, spout in di-
lute pha se is thus created, and pe netrates the center
region of the spo uted bed (Figur e 8.19). How ever, if a
fairly large jet replaces the co nical centra lly located jet
in a spou t bed , a jetting fluidized bed is form ed. One
distinct ive featu re of jetting flui dized bed is that
bubbles are formed inst ead of dilut e pha se spout
(Figur e 8.21). Small-s cale jetting fluidized beds have
been applie d in co ating and granula tion process es.
8.8.12 FLUIDIZED B ED DRYERS WITHINTERNAL BAFFLES
Internal baffles can be inserted into a fluidized bed to
divide the bed into several compartments. Various
types of baffles can be used, e.g., wire mesh, perfor-
ated plate, turn plate, louver plate, and ring [63]. In
efficien t baffled fluidized bed dryer can only be deter-
mined by carryin g out pilot test ing.
8.8.13 SUPERHEATED S TEAM F LUIDIZED BED DRYERS
Superhe ated steam as the fluidizin g medium offers a
number of advan tages, e.g. , no fire or explosi on ha z-
ards, no oxidat ive damage, bette r operatio n perfor m-
ance (highe r drying rate) and prod uct qua lity,
environm ental friend liness, high en ergy consu mption
efficien cy, suitabil ity for drying of prod ucts contai n-
ing toxic or expensi ve or ganic liqui ds, abili ty to per-
mit pa steurizat ion, sterilizati on, and deod orization of
food products [66,67]. Details are available elsewhere
in this handbook.
The application of superheated steam fluidized
bed dryer has been reported for drying of paper and
pulp, wood- based biofuels (F igure 8.23), sugar be et
pulp, and paddy [65,66]. Superheated steam fluidized
Exhaustgas
Jetadditio n, the internals can be placed horizont ally or
vertical ly (Figur e 8.22) . Horizo ntal ba ffles are fre-
quently used. The object ive of inserting baffles (hori -
zontal and vertical ) is to limit bubbl e grow th and
coales cence [64,65]. Hen ce, the baffled fluidized bed
Solids outGas inlet
FIGURE 8.21 Jetting fluidized bed dryer.is useful to proce ss group B an d D particles becau se
large bubbl es a re form ed with such partic les. The
effect of baffles on the ga s and so lids flow is v ery
complex and is de pendent on bed diame ter, distance
between baffles, baffle opening and operati ng co ndi-
tions. The optim um co ndition s for operatin g an
(a)
Solids
Gas in
Gas distributor
Horizontalbaffles
Bubbles
FIGURE 8.22 (a) Horizontal baffled fluidized bed dryer; (b) ver
2006 by Taylor & Francis Group, LLC.bed drying of foodstuff, coal, bagasse, sludges, spent
grains from breweries, lumber, tortilla, vegetables,
herbs, and spice is also possible [67,70].
8.8.14 FLUIDIZED BED FREEZE DRYER
Freeze-drying is one of the low-temperature drying
techniques suitable for drying of highly heat-sensitive
materials such as drugs, pharmaceutical, biological,
and food products. Freeze-drying removes mois-
ture captured inside the solids by sublimation of
moisture from solid state (ice) to vapor state.
Ordinary freeze-drying is carried out in vacuum.
Over the years, new developments showed that freeze-
drying can be carried out at atmospheric pressure
and as well as in a fluidized bed (e.g., Refs. [7173]).
Here the drying rate is very slow. Wolff and Gibert
[74] showed that fluidized bed freeze-drying at
(b)
Solids out
Gasin
in
tical baffled fluidized bed dryer.
compres sor. The co mpresso r raises the enthal py ofatmosp heric pre ssure wi th the use of adsorben ts can
increa se the drying rate ap preciab ly (abo ut seven fold
compared to that without ad sorbent ). In this case,
adsorbent particles play a dua l role as transfer ag ent
for both heat and mass trans fers. But there is diffi-
culty in separat ing adso rbent pa rticles and frozen
dried pr oducts at the en d of the process . It is thu s
suggest ed to use parti cles that are edible or compat -
ible with human consumpt ion su ch as starch. Fluid-
ized be d freeze-dryi ng assisted by adsorbent involv es
three stage s, namel y freez ing of pr oduct, subli ma-
tion of free-fr ozen water, and secondary dehy dration
by desorpt ion.
W olff and Giber t [75] suggested that fluidized bed
freeze-dryi ng sho uld be carried out at higher tempe ra-
ture, but low er than the freez ing point. They sho wed
that fluidized bed freez e-dryin g wi th ab sorbent co n-
tributes to about 35% saving in heat requir ement ,
respect ively, althoug h much longer drying tim e is
needed as compared to vacuum freeze-dryi ng.
8.8.15 HEAT P UMP F LUIDIZED B ED DRYER
Steamfrom dryer
Heat exchangerPressurized screws
Wet product
CondensateDistributor plateImpeller
Screw conveyor
Dry product
Fluidized bed
Steam supply
Cyclone
FIGURE 8.23 Pressurized superheated steam fluidized beddryer.An ord inary fluidized bed drying system consis ts of a
blower, heater , de humidifi er (opti onal), fluidized be d-
chamber, and cyclone, whereas an ord inary he at
pump drying system consists of evapo rator, compres -
sor, conden ser, and an exp ansion valve. By combin-
ing fluid ized bed and heat pump drying syst ems,
where the evaporat or acts as a de humidi fier an d the
conden ser as a heater , a hea t pum p fluid ized bed
dryer is formed .
The worki ng fluid (refrigerant) at low pr essure is
vaporiz ed in the evaporat or by heat draw n from the
exhaust humid air. At the same time, cond ensation of
moisture oc curs as the exhaust air temperatur e go es
below dew poi nt tempe rature . Thus, the proce ss air
is deh umidifi ed. The working fluid then goes to
2006 by Taylor & Francis Group, LLC.the workin g fluid an d dischar ges it as superheat ed
vapor at high pressur e. Heat is remove d from the
working fluid and retur ned to the process air, which
has been dehumidified previously at the condenser.
As a result, the process air temperature increases. The
working fluid is then throttled using an expansion
valve to the low-pressure line and enters the evapor-
ator to complete the cycle, whereas the dehumidified
and heated process air is charged into the fluidized
bed drying chamber to remove moisture of solids.
Details on heat pump drying are available elsewhere
in this handbook.
Figu re 8.24 shows a typical he at pum p fluidized
bed dryer. The fluidized bed drying chamber receives
wet solids and discharges dried product whereas de-
humidified and heated air is charged into the chamber
from the bottom of the chamber. The drying tempera-
ture can be adjusted by monitoring the capacity of
condenser, whereas the desired humidity of inlet air
can be obtained by controlling the motor frequency
of compressor.
The advantages offered by heat pump fluidized
bed dryer are: low energy consumption due to high
specific moisture extraction rate (SMER), high coef-
ficient of performance (COP), wide range of drying
temperature (20 to 1108C), environmental friendli-ness, and high product quality. Thus this type of
dryer is suitable for heat-sensitive products such as
food and products of bio-origin.
As chloroflurocarbons (CFC) and hydrochloro-
flurocarbons (HCFC) are to be phased out very soon,
working fluids such as carbon dioxide, ammonia,
R717, and R744 can be used as substitutes [76].
Many products have been tested at the Norwegian
Institute of Technology, such as food products, fish,
fruits, and vegetables [77,78].
8.9 DESIGN PROCEDURE
Design procedures for batch and continuous dryers in
constant and falling rate periods vary widely. The
discussion here is restricted to particulate solids drying.
8.9.1 DESIGN EQUATIONS
8.9.1.1 Residence Time
If the particles are small, very porous, and sufficiently
wet to contain free moisture, the drying rate remains
constant throughout the drying process. On the other
hand, if the solid particles initially contain surface
moisture, falling rate period will occur after a short
period of constant rate period. In this case, the design
calculation should include two steps: one for the
rr
hreconstant rate and the other for the falling rate. Table
8.4 sho ws the equ ations for calculati ng residence time
at different operating conditions.
8.9.1.2 Sizing of Bed
Dry solids
Wet solids
Externalcondense
Condense
T
FIGURE 8.24 Heat pump fluidized bed dryer.Sizing of bed is based on simple hold-up mass bal-
ance. Cross-sectional area of the fluidized bed can be
determined from the following equation after solids
flow rate (dry basis), Fs, bed density, rb, and bedheight, Hb, are specified, and particle residence time,
tR, is determined:
A FstRrbHb
(8:28)
8.9.1.3 Gas Flow Rate
Gas flow rate (dry basis) is calculated from the fol-
lowing equation. The operating gas velocity, ug, is
specified as a multiple of the minimum fluidization
velocity, normally it is 23umf for fluidized bed
drying. Anyway, the suitable operating gas velo-
city can be determined from laboratory-scale fluidized
bed testing as long as the gas velocity yields good
fluidization quality during the operation:
Gg rgugA (8:29)
where rg is the density of gas.
2006 by Taylor & Francis Group, LLC.8.9.1.4 Mass Balance, Continuous
Drying, Well-Mixed Bed
Fs(Xin Xout) Gg(Yout Yin) (8:30)
Compressor
e way valve
Receiver
Expansion valve
Evaporator
CondensationIn this equation, Fs is the solids flow rate (kg/s), X is
the moisture content (kg/kg), Gg is the gas flow rate
(kg/s), and Y is the absolute humidity (kg/kg).
8.9.1.5 Heat Balance, Continuous
Drying, Well-Mixed
Heat balance for the single-phase model gives the
following energy balance:
FsHsin GgHgin Qh FsHsout GgHgout Qw(8:31)
In this equation, Qh is the rate of heat input from
immersed tubes (kJ/s), Qw is the rate of heat loss from
wall (kJ/s), andH is the enthalpy (kJ/kg). Enthalpy of
solids at the inlet and outlet can be obtained from
Equation 8.32 and Equation 8.33, respectively:
Hsin (cps Xincl)Tsin (8:32)
Hsout (cps Xoutcl)Tsout (8:33)
D
TABLE 8.4Equations to Determine Residence Time Required for
Remarks
Batch Drying
1. Constant rate period Only surface moisture presentFor a gasvapo r system, Hg in and Hgout can beobtained from Mollier di agram and f or organic vapor
inert gas systems, Hg in an d H gout can be obtaine dfrom the followi ng eq uations :
Hg in (c pg Yin c 1 )T g in Yin l (8 : 34)
2. Falling rate period (i) From diffusion model
(ii) Simplified equation
(iii) Empirical formulation
Continuous drying
(a) Well-mixed Design curve:X 10X (t)E(t)dt [79]
1. Constant rate period Only surface moisture
2. Falling rate period
3. Batch drying curve (1) Obtain a record of the changing bed tem
(2) Divide the constant inlet air temperatur
increment note the time DtT1 required to
temperature of T1
(3) Calculate the time DtT2 required to acco
T2 by the use of the following equation:
DtT1DtT2
[(psat pin)(X Xe)]T1[(psat pin)(X Xe)]T2
[81,82]
(4) Build up the constant bed temperature b
(5) Obtain drying equation for each curve
(6) Obtain residence time from design curve
tR SAf *Gb
Xin XoutXout Xeq
[83,84]
where S is the bed loading, A is the bed are
at constant be temperature, T1
(b) Plug flow
1. Batch drying curve Residence time distribution function is E(t)
where
B DtmL2
and D 3:71 104(u umf )u1=3mf
[82]
D 1:49[0:01(Hb 0:05) 0:00165rs(u uu2=3mf
Note that validity of Reays correlation for
to 0.10m. There is some evidence in the lite
deeper beds [50]. Shallow bed is recommend
of solid particles in the bed
2006 by Taylor & Francis Group, LLC.rying
Drying Time Required
tR (Xo X )MslGgcpg(Tin Tout)Hg out ( c pg Yout c 1 )T g out Yout l (8 : 35)
A summ ary of steps for fluidized bed dryer de sign is
given in Figure 8.25, wher eas a sim ple g uide for
selecting suit able fluidized bed dryers (FBD) based
on mate rial propert ies is given in Fig ure 8.26.
X XeqXo Xeq
6
p2
X1n1
1
n2e[(np)
2Dt=R2]
tR is obtained by trial and error
tR MscpsGgcpg
lnTp TinTpo Tin
tR 1k lnXcr1 XeqX Xeq
tR Xo Xk
tR 1k
Xin XeqXout Xeq 1
[80]
perature Tb during constant inlet air temperature run
e batch drying curve X(t) into increments of length, DX. For each
accomplish that amount of drying at constant bed
mplish the same increment of drying at constant bed temperature,
atch drying curve by increments
a, f* is ratio of bed loading (S) and flux of gas flow rate (G/A)
12pB
p exp (1 t=tm)2
4B
" #
;
mf )]u0:23
[83]
particle diffusivity has only been confirmed for bed depths up
rature that D may be an order of magnitude larger in much
ed if the objective is a close approach to plug flow behavior
e F
ract
ch
mpee
rve
me,
anSetup laboratory-scal
Determine fluidization cha
Set ug, z, Tg, perform bat
Calculate constant bed tebatch drying curv
Determine design cu
Estimate residence ti
Fix bed geometry, Agas flowrate, Gg8.9.2 A SAMPLE DESIGN C ALCULATION
Wet particu late solid s (6000 kg/h) with an initial
moisture con tent of 20% (db) at 20 8 C are to be dr iedto fina l mois ture co ntent of 4% (db). Inlet air at
125 8 C with humidi ty of 0.005 kg/kg is used. Beddepth is 20 cm.
Un der these conditi ons, bed de nsity is 500 kg/m 3
and equili brium mois ture co ntent is zero . Specific
heat of the dry soli ds and liquid water are 1.0 and
4.2 kJ/kg 8 C, respect ively. Figu re 8.27 gives the sum-mary of all available data on this problem . Heat loss
at the wal l of the dryer is estimat ed as 5% of the heat
content of inlet air. Batch drying curve was obtaine d
at the co nditions mention ed abo ve; the relation ship
Check the requirement for: Cooling Good distributor design Efficient gas cleaning Reduction of entrainment High heat demand Justification due to low drying rate
Determine outlet gas humiditand dew point
Check RH, satisfactory
No
Optimize?
Yes
Check for risk of condensa
Yes
FIGURE 8.25 Design steps starting from laboratory tests.
2006 by Taylor & Francis Group, LLC.BD
eristics
drying
rature
tR
d
Changez, T between dr ying rate and mois ture content is given by
the foll owing equ ation:
dXdt 0: 005 X
Calculat e
(a) Mean pa rticle resi dence time
(b) Bed area
(c) Mass flow rate of air
(d) Absol ute humidity of e xhaust air
(e) Temp erature of exhaust air
(f) Check wheth er co ndensati on will occ ur in
cyclone
Stringent requirement for final moisture content
Recovering of valuable solvent Explosion hazard Toxic hazard Ignition hazard
y, Yout
? No
No
Change Gg
tion Yes
Change A, Gg
WM-FBD Well-mixed FBD SBD Spouted bed P-FBD Pulsating FBD H-FBD Hybrid FBD
PF-FBD Plug flow FBD M-FBD Multistage FBD IT-FBD Immersed tubes FBD IS-FBD Inert Solids FBD
V-FBD Vibrated FBD A-FBD Agitated FBD B-FBD Baffled FBD SD Spray drying
Group A, Bgood fluidizability particles
Group C, Dpoor fluidizability particles
Crystallinesurface moisture
Fragile Colloidal/poroussurface + internal moisture
Surface + internalmoisture
Heat-sensitive Heat-resistant Heat-sensitive Heat-resistant
Monosized
Monosized
Polydisperse
Polydisperse
Liquids; pastes
LiquidsGroup Cfine particles
Group Dlarge particles
Pastesslurries
Surfacemoisture
V-FBD
PF-FBD V-FBD WM-FBD
M-FBD V-FBD SBD
WM-FBD V-FBD SBD
V-FBD A-FBD IT-FBD
SBD V-FBD
H-FBD(spray-FBD)
M-FBD H-FBD (SD-slow), (FED-slow)
P-FBD
A-FBD SBD IS-FBD
B-FBD
V-FBD SBD SBD
FIGURE 8.26 Dryer selection.
2006byTaylor&Francis
Group,LLC.
WSolution
For continuous, well-mixed dryer operation in the
linear falling period, the residence time is given by
tR 1k
Xo XeqX Xeq
1 !
tR 10:005
0:20 00:04 0 1
tR 800 s
Dry solid mass flow rate is calculated from wet solid
mass flow rate, wet solid has initial moisture content
of 20%,
kg wet solid 1 kg dry solid 1 h
Dry solidsX = 0.04 kg/kg
BedHb = 20 cmrb = 500 kg/m3tR = ???A = ???Tb = ???
Exhaust air
Dry solid
FIGURE 8.27 Sample calculation.F 6000h
1:20 kg wet solid
3600 s
F 1:389 kg dry solid=s
Bed area is given by
A FstRrbHb
A 1:389 800500 0:20
A 11:11m2
Mass flow rate of air is calculated from the equation
Gg rgugA
2006 by Taylor & Francis Group, LLC.Gg 1:0 0:70 11:11
Gg 7:777 kg=s
Outlet air humidity can be obtained from the equation
Fs(Xin Xout) Gg(Yout Yin)
Yout FsGg
(Xin Xout) Yin
Yout 1:3897:777
(0:20 0:04) 0:005
Yout 0:0336 kg H2O=kg dry air
Outlet air temperature can be obtained from the
equation
Wet solidsFs = 6000 kg/hTs,in = 208CXo = 0.20 kg/kgrs = 2000 kg/m3cps = 0.84 kJ/kgK
Hot airug = 0.70 m/sYg,in = 0.005 kg/kgrg = 1 kg/m3cpg = 1.00 kJ/kgKTg,in = 125 8CGg = ???
et solid
Hot air orflue gasFsHsin GgHgin Qh FsHsout GgHgout Qw
Qh 0 since there is no immersed tube.Qw 0.05GgHgin assumes that heat loss to wall is
taken as 5% of the enthalpy of inlet air:
Hsin (cps Xinc1)TsinHsin (0:84 0:20 4:2) 20
Hsin 33:60 kJ=kgHsout (cps Xoutc1)TsoutHsout (0:84 0:04 4:2)T
Hsout 1:008T kJ=kg
Hgin (cpg Yinc1)Tgin Yinl
H (1:00 0:005 4:2) 125 0:005 2370
H height, m
p partial pressure, Pagin
Hgin 139:5 kJ=kg
Hgout (cpg Youtc1)Tgout Youtl
Hgout (1 0:0336 4:2)T 0:0336 2370
Hgout 1:141T 79:63
FsHsin GgHgin Qh FsHsout GgHgout Qw
FsHsin GgHgin Qh FsHsout GgHgout 0:05GgHgin
FsHsin 0:95GgHgin Qh FsHsout GgHgout
1:389 33:6 0:95 7:777 139:5 0 1:389 (1:008T) 7:777 (1:141T 79:63)
T 44:6C
From the psychrometric chart, air at absolute humid-
ity of 0.0336 kg/kg has a dew point of 33.58C andrelative humidity is 55%. Since the outlet air leaves
the dryer at 44.68C (108C higher than the dew point),there is no risk of condensation.
8.10 CONCLUSION
Fluidized bed dryers have replaced some of the con-
ventional dryers, e.g., rotary or conveyor dryers in
many instances. Among some of the recent develop-
ments in fluidized bed drying is the idea of applying
microwave energy field continuously or intermittently
in a fluidized or spouted bed. Use of superheated
steam will probably become more popular in some
applications in the future.
The presence of moisture on particle surface can
cause major changes to fluidization quality as com-
pared with that of dry particles to which most of the
available literature is applicable. Also, there are nu-
merous variants of the fluidized bed that require dif-
ferent design information and design strategies. For
example, drying using a time-dependent heat input or
drying under low-pressure conditions or using super-
heated steam as the drying medium, etc. must be
handled with some modifications and new data sets
and models.
NOTATION
a, b, x, y, k drying constant, drying coefficient
A area, m2
c heat capacity, J/(kg K) 2006 by Taylor & Francis Group, LLC.P pressure, Pa
Pr Prandtl number
q rate of heat transfer, W
Qh heat input from immersed tubes, kJ/s
Qw heat loss to column wall, kJ/s
r radius, m
Re Reynolds number
t time, s
T temperature, 8C, Ku velocity, m/s
V volume, m3
X moisture content, kg/kg
Y absolute humidity, kg/kg
GREEK SYMBOLS
b root of Bessel function void fractionl latent heat of vaporization, J/kgm viscosity, Ns/m2
r density, kg/m3
s StefanBoltzmann constant 5.67108 W/(m2 K4), W/(m2 K4)
f sphericity
SUBSCRIPT
b bed
bb bubble
c convective component
cr1 first critical
cyl cylinder
d denseh heat transfer coefficient, W/(m2K)
Kc mass transfer coefficient across bubble
boundary, m/s
k thermal conductivity, W/(m K)
L length, m
M mass, kg
_mm mass rate of evaporation of water perunit volume of bed, kg/(m3 s)
n integer
Nu Nusselt numbercp heat capacity at constant pressure
J/(kg K)
d diameter, m or mmD diffusivity, m2/s
e emissivity
E(u) residence time densityF solids mass flow rate, kg/s
g gravity acceleration 9.80665m/s2,m/s2G gas mass flow rate, kg/s
eff effective
Dekker, New York, 2003, chap. 6.
5. Mujumdar, A.S. and Devahastin, S., Applications for
11. Mersman, A., ZumWarmeubergang inWirbelschichtenf